Ken G said:
I wasn't aware that SR was more easily falsified than LET though, because they both make all the same predictions. I felt SR was favored more on Occam's razor-- if you don't need an aether, why have one? But if SR was proved wrong, and there is an "aether frame", then Lorentz' version would be wrong too.
It’s true that the Lorentzian ether interpretation and the spacetime interpretation are empirically equivalent for all presently known phenomena, but they stand differently in regard to falsifiability in the face of any future phenomena that might be discovered. In the etheristic interpretation, Lorentz invariance represents a large number of independent coincidental facts: electromagnetism happens to be Lorentz invariant, the strong nuclear force happens to be Lorentz invariant, mechanical inertia of every known elementary particle happens to be Lorentz invariant, and so on. There is no conceptual link between these (once the electromagnetic view of the world was ruled out), so for any new class of phenomena that might be discovered, the ether interpretation really gives no warrant to believe it would be Lorentz invariant. The ether can be given whatever properties it needs to conform with any new facts. Indeed this was Lorentz’s professed reason for continuing to prefer his interpretation. He said we shouldn’t relinquish the language of an absolute rest frame, because we might need it some day. In contrast, the spacetime interpretation takes all those coincidences and removes them from the individual phenomena, and accounts for them in terms of the Minkowskian structure of spacetime itself. In this interpretation, any new particle or interaction that might be discovered tomorrow is constrained to be (at least locally) Lorentz invariant. The only way the spacetime interpretation is viable is if (local) Lorentz invariance is universal and complete. If it fails for any phenomenon, then the single unified spacetime interpretation fails, and we must go back to treating the Lorentz invariance (or lack thereof) of each phenomena as an independent fact, as it is in the ether interpretation. It’s in this sense that the spacetime interpretation is much more exposed to falsifiability than is the etheristic interpretation. Think of all the new phenomena, interactions, and particles that have been discovered subsequent to 1905, not to mention the increase in the range of parameters explored by experiment. Any one of these new classes of phenomena or observations might have been found to violate (local) Lorentz invariance (think CERN neutrinos...) and rendered the spacetime interpretation unviable, but none of them did – not even the entanglement aspects of QM. But the Lorentzian framework would not have been invalidated by whatever might have been found.
Ken G said:
I'm not saying that there is something special about quantum postulates, I'm saying there is something special about postulates in the first place. The empiricist view is that all theories are approximate, so none of their postulates should be assumed to hold precisely.
But it isn’t necessary for any particular set of postulates to hold precisely in order for someone to espouse an MWI interpretation, is it? I think we agree that one could have an MWI of virtually any theory, so revising the postulates of QM wouldn’t necessarily drive someone away from MWI.
The question of whether we insist that our current theory is precisely correct, or whether we acknowledge that our current theory may be subject to future revision, is separate from the question of whether a many-worlds interpretation is useful or sensible. I think the espousal of MWI doesn’t necessarily commit someone to the position that the postulates of QM are precisely correct, nor does it imply that they would have to abandon MWI if/when the postulates of QM were revised.
Ken G said:
Since MWI is never falsifiable, it is only the motivation for it that is falsifiable (the aesthetic structure of the postulates).
I agree that if the experiential theory (in this case, QM) changed, it is conceivable that the revised theory might give people less – or more – motivation to think in terms of MWI. For example, Deutch thinks we could perceive the other worlds after all, and he would take this as proof positive of the reality of the many worlds. This would entail a revision of QM, but would actually (according to Deutsch) increase our motivation for MWI. Of course, one could also imagine changes to QM that would make MWI seem less plausible. So the fact that the postulates of QM might be revised at some point doesn’t really argue univocally either way, for or against MWI, because as a conceptual framework it has none of the rigidity of, say, the spacetime interpretation of special relativity. It is much more akin to an ether theory, that could accommodate any set of observations.
Ken G said:
It's very hard to say just what it is exactly about QM, rather than any other theory based on postulates, that supports an MWI approach, when no other theory ever did (though it could be argued that Parmenides, 2500 years ago, did in a sense suggest a similar theory, but it was pre-scientific).
I agree that it’s interesting to consider what motivates the MWI approach, and whether some experiential theories give more motivation than others, or if it is just an accident of fashion. Throughout history, people have contemplated the notion that the world of our experience is just one of many “possible worlds”, along with the ancient idea that every mathematical form has physical meaning. Ideas like this have been around forever. Remember Leibniz discussing what sounds a lot like the principle of least action (his Born rule), asserting that we live in “the best of all possible worlds”, which is quite similar to how many modern advocates of MWI conceive of things, i.e., possible worlds rather than actual worlds.
The notion of multiple possible worlds (and counterfactual definiteness, etc) arises in any theory based on differential equations. Newton and his contemporaries were acutely aware of this “deficiency” in any such theory, and some even argued that Newton’s “mathematical principles” were non-scientific and vacuous, complaining that a theory such as Newton’s tells us nothing that is not already implicit in the initial conditions, which must be put in by hand. It’s difficult for us to grasp this today, but when the idea of a differential equation representing a physical theory was new, it was not immediately accepted as even accomplishing anything. The equations of Newtonian mechanics may be said to imply a giant phase space, within which our universe is represented by a single trajectory, so it is a superb descriptive tool, but the theory doesn’t tell us WHICH trajectory in this enormous phase space is THE trajectory of THE universe, which is what many people regarded as the main task of a theory of natural philosophy. In Newton’s theory we have to specify a full set of initial conditions, sufficient to fully define everything of interest (per Laplace’s vision of determinism). This specification provides nearly ALL the information of the theory, and yet it is purely ad hoc and separate from the differential equations that supposedly define the theory. This could easily lead someone to eschew the task of specifying THE trajectory, and simply take the equations themselves as the entire theory, which entails ALL possible trajectories within the phase space. This certainly yields a more symmetrical and less ad hoc interpretation... but it's also sterile and pointless.
Ken G said:
We certainly encountered lack of complete information in theories before, like in thermodynamics. I think it was the discovery of a fundamental limit on information, the HUP, that is the real source of MWI...
I agree that the inherent uncertainty in QM is what leads to the extra motivation for MWI. The key difference between Newtonian mechanics and quantum mechanics (for motivating MWI) is that in Newtonian mechanics the equations of motion range only over the set of observable states, so there is no ambiguity when translating from the variables in the equations to the measures of our experience, whereas in quantum mechanics the equations of motion range over the set of superpositions of observable states. People tried hard to avoid this, and to come up with equations that range only over observable states, but eventually it came to be seen as an impossible task. Quantum phenomena apparently cannot be modeled effectively except by equations that range over superpositions of observable states. This means that an extra step is required when going from the variables of the equations of motion to an actual observed outcome. This is the “collapse of the wave function”, in accord with the Born rule, and the special challenge for interpreting quantum mechanics is how to conceive of this extra step, selecting just one trajectory through phase space, and calling it OUR trajectory. But this is not really as different as it might seem from the extra step that is required in Newtonian clockwork mechanics, i.e., the stipulation of initial conditions, which essentially represents a collapse from the set of all possible trajectories down to the single trajectory that we experience. The difference is that Newtonian mechanics requires only one “collapse” step, because for any given exact specification of the state, the equations of motion give exact specifications of all subsequent (and prior!) observable states. Hence we never need to repeat the collapse step, and we can set aside the single collapse step and not worry about it too much. In contrast, because of the inherent uncertainty in QM, after stipulating an initial state, the equations of motion lead to a superposition, and even if we stipulate an observation and update our state, the equations of motion again lead to a superposition, and so on. Thus we encounter the need for collapse repeatedly, making it more difficult to ignore. But it isn’t a qualitative difference, it’s just a quantitative difference, relative to the collapse required in Newtonian mechanics.
Ultimately I think a MWI is no more useful for QM than it is for Newtonian mechanics. We can always imagine that the world of our experience is embedded in a larger structure of other worlds, but if this imagined embedding doesn’t tell us anything new about the world of our experience, then it’s pointless.